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sustainability

Article Indicators for Size Distributions of Airborne Particles and Traffic Activities in Urban Areas

Jin Yong Jeon 1, Joo Young Hong 2,* , Sung Min Kim 1 and Ki-Hyun Kim 3

1 Department of Architectural Engineering, Hanyang University, Seoul 04763, Korea; [email protected] (J.Y.J.); [email protected] (S.M.K.) 2 School of Electrical & Electronic Engineering, Nanyang Technological University, Singapore 639798, Singapore 3 Department of Civil and Environmental Engineering, Hanyang University, Seoul 04763, Korea; [email protected] * Correspondence: [email protected]; Tel.: +65-8429-7512

 Received: 6 November 2018; Accepted: 29 November 2018; Published: 5 December 2018 

Abstract: The aim of this study was to explore the relationships among the particle number concentration (PNC), noise, and traffic conditions. Field measurements were conducted to measure the temporal variabilities of the noise levels and PNC over 24 h in a location adjacent to three main traffic in Seoul, Korea. The PNC was measured in the range of 0.3 to 10 µm. The noise data was measured by utilizing both the overall levels and spectral characteristics. Traffic data including volumes and speeds of vehicles on the roads were also collected. The results showed that the correlations among the three key parameters varied depending on changes in the noise and particle size. The noise levels at 100–200 Hz were positively correlated with traffic volume and submicron particles. In contrast, they exhibited inverse correlations with the traffic speed and the number of larger particles (>2.5 µm). Compared to noise levels at 100–200 Hz, noise levels at 1–2 kHz exhibited reverse relationships between the traffic and PNC. Submicron particles (0.3–1.0 µm) tended to be more strongly associated with noise levels during the daytime, while those greater than 2.5 µm maintained relatively stable correlations with the noise throughout the day. The findings address the importance of temporal and spectral-specific monitoring of air and noise for a better understanding of the exposure of the community to air and noise .

Keywords: noise pollution; ; particle number concentration; traffic; diurnal pattern; urban built environment

1. Introduction Urban dwellers are exposed to multiple pollutants such as noise, light, and air pollutants; the exposure to combined environmental pollutants could increase the risk of adverse effects on human health and well-being [1]. Among the pollutants, as verified by extensive evidence, noise [2,3] and air [4,5] adversely affect human health. Epidemiological studies have demonstrated convincing associations between particulate air pollution and human health problems including cardiovascular, and respiratory diseases [4–8]. In particular, particulate pollutants, which consist of a heterogeneous mixture of particles suspended in air characterized by particulate matter (PM) and the particle number concentration (PNC), are associated with adverse human health effects [4,8–14]. Environmental are also known to potentially cause not only noise-induced hearing impairment [3,15], but also non-auditory health problems [16]. Apart from hearing impairment, noise exposures have physiological effects such as mental stress, cardiovascular problems, and effect over the sense of balance [17,18]. Acute noise exposures can increase blood , heart rate,

Sustainability 2018, 10, 4599; doi:10.3390/su10124599 www.mdpi.com/journal/sustainability Sustainability 2018, 10, 4599 2 of 19 and vasoconstriction by activating the autonomic and hormonal systems [16,19]. Chronic noise exposure can potentially cause and heart disease in vulnerable individuals [20–23]. Additionally, causes annoyance, speech interference, sleep disturbance, and reduced performance of cognitive tasks in living spaces [21,24–31]. Perceived acoustic quality are also closely associated with mental health outcomes (e.g., psychological distress, incidence of anxiety, and depression) [32]. Accordingly, WHO Regional Office of Europe provides recommendations for protecting human health from exposure to environmental noise from various sources: transportation, wind turbine, and recreation [2]. In urban settings, vehicular traffic activities play an important role as a common source of both noise and air pollution [6,33–35]. There have been a number of studies investigating the relationships between environmental noise and air pollutants in urban areas [23,36–42]. Some studies have investigated the temporal correlations between air pollution and noise levels [40,42,43]. The temporal patterns of air pollutants including the mass/number concentrations of particulate matter and/or organic/inorganic compounds have been investigated in many previous studies to determine their associations with noise levels [40,42–45]. In terms of particulate pollutants, the particle mass fractions PM 10 and PM 2.5 are widely used. Although the PNC is not typically regulated, recent studies showed that the PNC associated with traffic conditions can be a significant indicator for health problems [11,12,46–48]. Nonetheless, relatively little is known about the temporal relationship between the PNC and noise [43,49]. In many previous studies, noise and air pollution data were usually monitored at distant locations, which may have complicated the interpretation of the relationships between noise, air pollution, and traffic. In addition, regarding noise metrics, studies investigating the relationships between noise and air pollutions primarily adopted equivalent noise levels representing the overall level of noise to examine the association with air pollution [37,43,47]. Despite the fact that the spectral variation of traffic noise varies depending on traffic speeds and the type of vehicles [50,51], only a few studies have dealt with noise parameters while investigating the frequency characteristics of noise to explore the relationships with air pollution [42,44,45]. In this context, the aims of this study are to explore the temporal correlations between traffic, noise, the PNC in urban areas, and to assess noise spectra indicators related to the particle size distribution to account for the status of air pollution. To achieve these goals, the noise conditions and PNC for various particle size fractions were measured concurrently in Seoul, Korea.

2. Methods

2.1. Measurement Location The measurement location and neighboring geographical conditions are illustrated in Figure1. The measurement of both noise and particle number was performed on a deck on the second floor of the Civil Engineering Building at Hanyang University, Seoul, Korea. The measurement unit was approximately 10 m above ground. The measurement site was exposed to air and noise pollutants from representative urban transportation systems including, different sizes of sections and a metro lane. As shown in Figure1, the measurement location is surrounded by three main road sections (T1–3) and one metro railway lane (M). The Sageundong road section, T1 (four lanes) and Wangsimni road section, T2 (six lanes), are 36 m and 42 m away from the measurement unit, respectively. The Dongbu Expressway road section, T3 (10 lanes), an expressway, runs nearly parallel to the measurement unit and the distance between the measurement unit and T3 was approximately 330 m. There is a city stream, namely Joong-rang Cheon, between T3 and the measurement point. Additionally, the metro lane (M), which runs parallel to T2, is immediately adjacent to the measurement unit. According to the Seoul Metro, subway trains utilizing normal braking and regenerative braking operate on the metro lane. On average, five subway trains run per minute. Although the metro trains run on electricity, which does not generate as much pollution as road traffic, brake pad wear can be a particulate matter Sustainability 2018, 10, x FOR PEER REVIEW 3 of 18

Sustainability 2018, 10, 4599 3 of 19 generator [44]. Other sources (e.g., industrial facilities) for noise and air pollutants were not located near the study area. Sustainability 2018, 10, x FOR PEER REVIEW 3 of 18

Figure 1. Field measurement area and conditions (source: http://map.naver.com). (a) Birdseye view and (b) aerial map of the measurement location. ‘T’, ‘M’, and ‘P’ indicate the traffic road, metro lane, and measurement unit, respectively. T1 (four lanes), T2 (six lanes), and T3 (ten lanes) are 36 m, 42 m, 330 m away from the measurement unit, respectively. M (two lanes) is immediately adjacent to the measurement unit.

2.2. Measurement Equipment and Setup

FigureFigure 1. 2 Field shows measurement the measurement area and traffictraffic devices conditionscondit andions se (source:(source:t-up on http://map.naver.comhttp://map.naver.com). the site. The environmental). ( (aa)) Birdseye Birdseye noise, mainlyview from and ( roadb) aerial traffic, map of was the measuredmeasurement measurement using location. a type ‘T’, ‘T’, ‘M’,2 ‘M’, sound and and ‘P’ ‘P’level indicate indicate meter the the (SVANtraffic traffic road, road, 953, metro metro Svantek, Warsaw,lane,lane, Poland)and measurement according unit,unit, to ISO respectively.respectively. 1996-2 [52]. T1 T1 (four (four The lanes), soundlanes), T2 T2level (six (six lanes),meter lanes), and(SLM) and T3 T3 (tenwas (ten lanes) mounted lanes) are are 36 on 36 m, am, 42tripod at a height42m, m, 330 330 mof awaym1.5 away m from and from thethe the measurement microphone measurement unit, of unit, the respectively. SLrespectiM wasvely. Mcovered (twoM (two lanes) by lanes) a is windscreen. immediately is immediately adjacentTotal adjacent particle to the to size distributionsthemeasurement measurement were unit. measuredunit. using a Class I laser-based handheld airborne particle counter (AeroTrak APC-9306, TSI Inc., Shoreview, MN, USA). The particle counter was located at the same 2.2. Measurement Equipment and Setup 2.2.height Measurement of the SLM. Equipment The measurement and Setup of noise levels and PNC was conducted on Tuesday 18:00 8th– WednesdayFigure 2 2 shows18:00 shows 9th the the December measurement measurement 2015 devices (24devices h) and under and set-up secleart-up on theweather. on site. the The site.The environmental Thenoise environmental levels noise,and airborne mainly noise, mainlyfromparticle road fromcounter traffic, road data was traffic, were measured waslogged usingmeasured with a typea step using 2 soundof 10a types leveland 2 averaged meter sound (SVAN level every 953,meter 5-min. Svantek, (SVAN Warsaw, 953, Svantek, Poland) Warsaw,accordingIn the Poland)to same ISO manner,according 1996-2 [52 meteorological to]. TheISO 1996-2 sound [52]. leveldata, The meterinclud sound (SLM)ing level the was wind meter mounted speed, (SLM) temperature, onwas a mounted tripod at and on a height arelative tripod of at1.5humidity a mheight and the(RH),of 1.5 microphone mwhich and thehave ofmicrophone thebeen SLM commonly was of the covered SL measuredM bywas a windscreen.covered in related by a Totalwindscreen.studies, particle were Total size simultaneously distributionsparticle size distributionswerecollected measured every were using10 smeasured using a Class a I portable laser-basedusing a thermo-hygro-anemometer Class handheld I laser-based airborne particlehandheld (Kestrel counter airborne Meter (AeroTrak particle4500NV, APC-9306, counterKestrel (AeroTrakTSIInstruments, Inc., Shoreview, APC-9306, Boothwyn, MN, TSI PA USA).Inc., USA), Shoreview, The and particle the MN,data counter wereUSA)was averaged. The located particle every at counter the 5-min same wasfor height analysis. located of the atIn SLM. theaddition, same The heightmeasurementduring of the the sampling SLM. of noise The period, levelsmeasurement traffic and PNCfrom of wasnoisethe three conducted levels main and traffic onPNC Tuesday roads was conducted (T1–3) 18:00 were 8th–Wednesday on recorded Tuesday using 18:00 18:00 video 8th– 9th WednesdayDecembercamcorders 2015 to18:00 calculate (24 9th h) underDecember traffic clear volumes. 2015 weather. (24 Using h) The underthe noise video clear levels recording, weather. and airborne the The hourly particlenoise traffic levels counter volume and data airborne of werelight particleloggedand heavy withcounter vehicles a step data of were were 10 s counted andlogged averaged forwith each a every step traffic of 5-min. 10 road. s and averaged every 5-min. In the same manner, meteorological data, including the wind speed, temperature, and relative humidity (RH), which have been commonly measured in related studies, were simultaneously collected every 10 s using a portable thermo-hygro-anemometer (Kestrel Meter 4500NV, Kestrel Instruments, Boothwyn, PA USA), and the data were averaged every 5-min for analysis. In addition, during the sampling period, traffic from the three main traffic roads (T1–3) were recorded using video camcorders to calculate traffic volumes. Using the video recording, the hourly traffic volume of light and heavy vehicles were counted for each traffic road.

Figure 2. Measurement spot (left) and the recording set-upset-up ((rightright)) onon thethe site.site.

In the same manner, meteorological data, including the wind speed, temperature, and relative humidity (RH), which have been commonly measured in related studies, were simultaneously collected

Figure 2. Measurement spot (left) and the recording set-up (right) on the site. Sustainability 2018, 10, 4599 4 of 19 every 10 s using a portable thermo-hygro-anemometer (Kestrel Meter 4500NV, Kestrel Instruments, Boothwyn, PA USA), and the data were averaged every 5-min for analysis. In addition, during the sampling period, traffic from the three main traffic roads (T1–3) were recorded using video camcorders to calculate traffic volumes. Using the video recording, the hourly traffic volume of light and heavy vehicles were counted for each traffic road.

2.3. Indicators for Noise, Particle Numbers, and Traffic Various noise indicators describing the level as well as the spectral and temporal structure of the noise were calculated in this study. Unweighted noise levels were used to calculate the noise parameters in this study because unweighted noise levels exhibit stronger correlations with traffic and air pollution than A-weighted noise levels [42]. The equivalent sound pressure level (Leq) was calculated to describe the overall noise level. Percentile sound pressure levels including L10, L50, and L90 were used to describe the temporal characteristics of the noise. In terms of the spectral characteristics of traffic noise, three noise parameters, LOLF, LHLF, and LHF-LF, were employed to describe the noise emission from road vehicles based on the noise measurements in the one-third octave band spectra from a previous study [44]. LOLF is the sum of the 100 to 200 Hz one-third octave band, which is developed to access the noise of road vehicles because in general, engine noise is dominant at low . LHLF, calculated as the sum from 1 kHz to 2 kHz, is related to rolling noise, which contains higher energy at high frequencies and higher speeds. LHF-LF is the difference between LHLF and LOLF, representing the high frequency content of noise. In terms of air pollutants, the optical particle counter utilized for this measurement enabled us to monitor size-segregated PNCs ranging from 0.3 to >10 µm with six different particle sizes during the sampling period. The particle sizes of the PNCs were divided into six different size ranges of 0.3–0.5, 0.5–1.0, 1.0–2.5, 2.5–5.0 µm, 5.0–10.0 µm, and >10.0 µm, similar to a previous study [53]. The traffic volume data aggregated by the number of vehicles per hour was calculated based on the video recordings during the measurement period. The hourly line-specific traffic density data was considered for both road directions of each road. The internet-posted traffic speed for each road section during the measurement period on the website of the urban traffic information system of Korea (www.utis.go.kr) were utilized.

2.4. Data Analysis In order to explore the relationship among the noise, PNC, and traffic metrics, Pearson’s correlation coefficients and multiple linear regression analyses were conducted. Based on the measured data, values averaged for 5 min over the sampling period were used to calculate the correlation coefficients among the noise parameters, PNC, and meteorological conditions. Meanwhile, the correlations with traffic parameters were analyzed using hourly data. All statistical analyses in this study were performed using the SPSS version 19.0 software. Since the hourly traffic speed and volume were collected from traffic roads (T1–3), the hourly averaged data with the corresponding standard deviations for noise indicators, PNCs, and meteorological parameters were plotted to compare with the temporal patterns of the traffic metrics.

3. Results

3.1. Temporal Patterns of the Noise Levels

The noise level data measured over 24 h is shown in Figure3. The measured Leq ranged from 69.5 dB and 94.5 dB throughout the day where the mean Leq was 79.4 dB. The diurnal patterns of Leq and percentile levels including L10, L50, and L90 for the measurement period are illustrated in Figure3a to understand the temporal trends of the noise levels each hour. The temporal patterns of the noise indicators can be divided into three main periods (Period 1 = 07:00–19:00, Period 2 = 19:00–22:00, Period 3 = 22:00–07:00). The divided time periods correspond to the daytime, evening, and night Sustainability 2018, 10, 4599 5 of 19 according to the European Environmental Agency (EEA). Table1 summarizes the measured noise indicators across three measurement periods. Significant changes of the SPLs were found in Periods 1 and 2. Overall, the Leq values dramatically increased after 07:00 due to the rush traffic period and reached 90.0 dB at 13:00, while the noise levels began to decrease to 80.2 dB between 13:00 to 15:00. Regarding the temporal variability of noise environment in Period 1, the differences among the percentile noise levels gradually increased such that the mean L10−L90 value was approximately 12.1 dB. Those findings imply that pronounced traffic activities may produce not only high noise levels but also various intrusive sound events such as horns during Period 1, which are normally considered to be working hours. In addition, it was observed that Leq precipitously increased after 15:00 and peaked at 18:00 with a value 90.7 dB due to the evening rush period. After working hours (Period 2), both overall noise level and temporal variance rapidly declined. In contrast to the tendencies in Periods 1 and 2, there are moderate changes in the sound pressure levels (SPLs). Overall, Leq was 72.6 dB (SD = 1.7 dB) in Period 3, where the variance of the SPLs reached a steady state compared to the other periods. With regards to the temporal structure of noises, the difference between the L10 and L90 values in Period 3 was relatively smaller than the other periods with a value of approximately 5.5 dB. This reflects that the traffic volume was constant with few noise sources excluding traffic such as human activities. Figure3b shows the temporal patterns of the SPLs in a 1/3 octave band from 63 Hz to 2 kHz. The diurnal trends of the SPLs band were different across the frequency band. It was found that high frequencies over 1 kHz showed moderate changes over the measurement period. The Leq values at 1 kHz and 2 kHz remained stable between 55 dB and 60 dB for the sample period. Unlike high frequencies, the variations of the SPLs at low frequencies below 250 Hz were greater than those at high frequencies. Significant increments of the SPLs at low frequencies (63–250 Hz) were observed in Periods 1 and 2, whereas the SPLs were relatively constant in Period 3.

Table 1. Summary of the noise parameters across the measurement periods. Period 1 = 07:00–19:00, Period 2 = 19:00–23:00, Period 3 = 23:00–07:00.

Noise Parameters [dB]

Period Leq L90 L50 L10 LOLF LHLF LHF-LF P1 Mean 83.5 74.4 79.2 86.5 68.2 61.0 −7.2 Min 73.6 70.4 73.5 75.5 60.4 58.7 −13.9 Max 94.5 81.1 88.9 98.3 73.7 63.8 1.9 SD 5.8 2.1 4.0 6.2 2.5 1.0 2.9 P2 Mean 80.9 72.8 77.1 84.0 68.6 60.8 −7.8 Min 74.9 70.2 72.8 77.1 64.1 59.0 −11.3 Max 89.1 76.2 82.6 92.3 71.8 62.6 −2.7 SD 3.3 1.3 2.0 3.5 1.9 1.0 1.9 P3 Mean 72.6 69.2 71.5 74.7 61.4 62.3 0.9 Min 69.5 66.5 68.1 70.9 55.6 59.8 −9.1 Max 79.9 72.6 76.3 83.4 71.2 64.1 7.8 SD 1.7 1.3 1.5 2.0 4.1 1.0 4.2 Total Mean 79.4 72.4 76.3 82.1 66.0 61.4 −4.6 Min 69.5 66.5 68.1 70.9 55.6 58.7 −13.9 Max 94.5 81.1 88.9 98.3 73.7 64.1 7.8 SD 6.6 2.9 4.6 7.2 4.5 1.2 5.1 Sustainability 2018, 10, x FOR PEER REVIEW 5 of 18 imply that pronounced traffic activities may produce not only high noise levels but also various intrusive sound events such as car horns during Period 1, which are normally considered to be working hours. In addition, it was observed that Leq precipitously increased after 15:00 and peaked at 18:00 with a value 90.7 dB due to the evening rush period. After working hours (Period 2), both overall noise level and temporal variance rapidly declined. In contrast to the tendencies in Periods 1 and 2, there are moderate changes in the sound pressure levels (SPLs). Overall, Leq was 72.6 dB (SD = 1.7 dB) in Period 3, where the variance of the SPLs reached a steady state compared to the other periods. With regards to the temporal structure of noises, the difference between the L10 and L90 values in Period 3 was relatively smaller than the other periods with a value of approximately 5.5 dB. This reflects that the traffic volume was constant with few noise sources excluding traffic such as human activities. Figure 3b shows the temporal patterns of the SPLs in a 1/3 octave band from 63 Hz to 2 kHz. The diurnal trends of the SPLs band were different across the frequency band. It was found that high frequencies over 1 kHz showed moderate changes over the measurement period. The Leq values at 1 kHz and 2 kHz remained stable between 55 dB and 60 dB for the sample period. Unlike high frequencies, the variations of the SPLs at low frequencies below 250 Hz were greater than those at highSustainability frequencies.2018, 10 ,Significant 4599 increments of the SPLs at low frequencies (63–250 Hz) were observed6 of in 19 Periods 1 and 2, whereas the SPLs were relatively constant in Period 3.

Figure 3. Temporal patterns of the SPLs: (a) Leq and percentile levels and (b) spectral characteristics of Figure 3. Temporal patterns of the SPLs: (a) Leq and percentile levels and (b) spectral characteristics noises. The error bars indicate standard deviations. of noises. The error bars indicate standard deviations. 3.2. Temporal Patterns of Road Traffic Data

The temporal variation in traffic volume (vehicle/hour, v/h) over the measurement period from three different road sections and the metro lane are plotted in Figure4. According to the Korea traffic noise prediction model (KHTN), the vehicles were classified into two types: heavy (gross vehicle weight ≥ 2.5 t) and light (gross vehicle weight < 2.5 t) vehicles. As shown in Table2, the percentages of light and heavy vehicle types for the three road sections were similar across the measurement period. The proportion of light vehicles was more than seven times higher than that of heavy vehicles across the three road sections. The standard deviations of the traffic volumes of light and heavy vehicles for T1 and T2 were approximately 6%, while that for T3 was approximately 4%, indicating that the proportions of light and heavy vehicle types for the three road sections were consistent across the measurement period.

Table 2. Percentages of vehicle types on the three road sections over the measurement period.

Road T1 T2 T3 Vehicle Type Light Heavy Light Heavy Light Heavy Mean 88.0% 12.0% 89.9% 10.1% 92.6% 7.4% SD 6.3% 6.6% 6.2% 6.4% 3.5% 3.9% Sustainability 2018, 10, x FOR PEER REVIEW 7 of 18

train was much smaller than that on the three main road sections. The subway operation hours in Seoul are from 5:30 to approximately 24:00 and the number of subway trains passing by the measurement location varied depending on the time of the day. The number of trains gradually increased from 6:00 until peaking at 8:00–9:00 based on the morning rush, then decreased from 10:00– 12:00 before peaking again at the evening rush from 19:00–20:00.

Table 3. Summary of vehicle types on the three road sections over the measurement period. Period 1 = 07:00–19:00, Period 2 = 19:00–23:00, Period 3 = 23:00–07:00.

Road T1 T2 T3 Period Vehicle Type Light Heavy Light Heavy Light Heavy P1 Sum 464 16 2377 47 18,440 1432 Min 12 0 212 0 2270 195 Max 156 12 856 20 6934 418 Mean 92.8 3.2 475.4 9.4 3688.0 286.4 SD 55.0 5.2 245.1 8.4 1875.1 85.3 P2 Sum 8888 1660 19,206 3318 90,031 8633 Min 137 31 493 47 5263 550 Max 1184 265 2716 416 9650 1265 Mean 808.0 150.9 1746.0 301.6 8184.6 784.8 SD 327.5 68.0 595.5 113.7 1138.6 221.1 P3 Sum 5612 784 12,295 1337 63,293 2995 Min 262 26 971 37 6209 249 Max 1085 194 1972 300 9573 609 Mean 701.5 98.0 1536.9 167.1 7911.6 374.4 SD 309.3 56.8 319.8 110.9 1248.6 128.6 Total Sum 14,964 2460 33,878 4702 171,764 13,060 Min 12 0 212 0 2270 195 Max 1184 265 2716 416 9650 1265 Sustainability 2018, 10, 4599Mean 623.5 102.5 1411.6 195.9 7156.8 544.2 7 of 19 SD 394.8 79.2 667.3 150.2 2229.1 282.4

FigureFigure 4. Temporal 4. Temporal patterns patterns of of the the traffic traffic volume:volume: ( (aa) )T1, T1, (b ()b T2) T2 (c) ( cT3) T3and and (d) (Subwayd) Subway train. train.

TableThe3 shows temporal the variations measured in traffic traffic indicatorsspeed for each across road three section measurement are plotted in periods. Figure 5. The The total traffic traffic volumespeed on data the per expressway, hour for the namely three main T3 road (mean sections = 7701.0, during SD the = sampling 2320.1), period was approximately were collected from 10.6 and 4.8 timesa website greater provided than thatby the on urban T1 (mean traffic =informatio 726.0 v/h,n system SD = 464.7of Korea v/h) (www.utis.go.kr). and T2 (mean The = 1607.5 mean v/h, traffic speed on T3 over the sampling period was 77.9 km/h, while those on T1 and T2 were relatively SD = 795.9 v/h), respectively. The road traffic parameters can also be explained by the three time periods (Periods 1–3) defined in the data.

Table 3. Summary of vehicle types on the three road sections over the measurement period. Period 1 = 07:00–19:00, Period 2 = 19:00–23:00, Period 3 = 23:00–07:00.

Road T1 T2 T3 Period Vehicle Type Light Heavy Light Heavy Light Heavy P1 Sum 464 16 2377 47 18,440 1432 Min 12 0 212 0 2270 195 Max 156 12 856 20 6934 418 Mean 92.8 3.2 475.4 9.4 3688.0 286.4 SD 55.0 5.2 245.1 8.4 1875.1 85.3 P2 Sum 8888 1660 19,206 3318 90,031 8633 Min 137 31 493 47 5263 550 Max 1184 265 2716 416 9650 1265 Mean 808.0 150.9 1746.0 301.6 8184.6 784.8 SD 327.5 68.0 595.5 113.7 1138.6 221.1 P3 Sum 5612 784 12,295 1337 63,293 2995 Min 262 26 971 37 6209 249 Max 1085 194 1972 300 9573 609 Mean 701.5 98.0 1536.9 167.1 7911.6 374.4 SD 309.3 56.8 319.8 110.9 1248.6 128.6 Total Sum 14,964 2460 33,878 4702 171,764 13,060 Min 12 0 212 0 2270 195 Max 1184 265 2716 416 9650 1265 Mean 623.5 102.5 1411.6 195.9 7156.8 544.2 SD 394.8 79.2 667.3 150.2 2229.1 282.4

As shown in Figure4a–c, the traffic volume significantly increased starting at 6:00 and peaked from 7:00–09:00 for T1 (1212 v/h), T2 (2040 v/h), and T3 (9744 v/h) because of the morning traffic rush. During main working hours (Period 1), the traffic volumes on T1 and T2 were constant but that on Sustainability 2018, 10, 4599 8 of 19

T3 fluctuated slightly and decreased from 15:00–18:00. In Period 2, the traffic on T1 and T2 gradually declined, while the traffic volume on T3 increased again after the evening rush period. Peak hour traffic volumes in the afternoon for T1–3 were 10,572 v/h, 1248 v/h, and 2652 v/h, respectively. In Period 3, the traffic volume on T1 dramatically decreased just after midnight and remained the lowest from 1:00 to 4:00 for all of the traffic roads. The traffic volumes on T1 and T2 during Period 3 were also the smallest over the sampling period. As shown in Figure4d, the traffic related to the subway train was much smaller than that on the three main road sections. The subway operation hours in Seoul are from 5:30 to approximately 24:00 and the number of subway trains passing by the measurement location variedSustainability depending 2018, 10 on, x theFOR timePEER REVIEW of the day. The number of trains gradually increased from8 6:00 of 18 until peaking at 8:00–9:00 based on the morning rush, then decreased from 10:00–12:00 before peaking again at theslow evening with values rush from of 25.3 19:00–20:00. km/h and 37.4 km/h, respectively. The temporal variance of the traffic speed onThe T3 temporal (SD = 4.2 km/h) variations was relatively in traffic smaller speed than for eachthose road on T1 section (SD = 6.8 are km/h) plotted and inT2 Figure(SD = 6.45. km/h). The traffic speed dataIn perPeriod hour 1, forthe thetraffic three speed main on roadT2 decreased sections significantly during the samplingfrom 45.0 km/h period to were23.5 km/h collected due to from a the morning rush (06:00–09:00) and almost constant traffic speeds were recorded with a value of website provided by the urban traffic information system of Korea (www.utis.go.kr). The mean traffic approximately 34.3 km/h. The traffic speed on T3 showed a similar temporal tendency with that on speed on T3 over the sampling period was 77.9 km/h, while those on T1 and T2 were relatively slow T2 during the period of 09:00–20:00, while a sudden increment of the traffic speed was observed withduring values Period of 25.3 2 km/h (20:00–21:00). and 37.4 In km/h, general, respectively. the traffic speeds The temporal in Period variance 3 were higher of the than traffic the speed other on T3 (SD =periods 4.2 km/h) for all was of the relatively traffic roads. smaller than those on T1 (SD = 6.8 km/h) and T2 (SD = 6.4 km/h).

FigureFigure 5. 5.Temporal Temporal patterns of of the the traffic traffic speed. speed.

3.3.In Period Temporal 1, Patterns the traffic of the speed Particle on Concentration T2 decreased and significantlyMeteorological Data from 45.0 km/h to 23.5 km/h due to the morning rush (06:00–09:00) and almost constant traffic speeds were recorded with a value of The particle number size distributions in six size ranges (0.3 to >10 µm) were collected during approximatelythe measurement 34.3 km/h. period The as trafficshown speedin Table on 4. T3 The showed hourly a averaged similar temporal values of tendency the particle with number that on T2 duringsizes the are period shown of in 09:00–20:00, Figure 6. It whilewas found a sudden that the increment diurnal tendencies of the traffic of the speed measured was observed PNC were during Perioddifferent 2 (20:00–21:00). depending In on general, the particle the size. traffic In speedsgeneral, in there Period are two 3 were temporal higher patterns than the for other the particle periods for all ofsizes. the traffic Smaller roads. particles between 0.3 and 1.0 µm tended to decrease during the periods of 0:00–02:00 and 21:00–23:00 and tended to peak around noon (11:00–12:00). In contrast to the smaller particles, 3.3. Temporalthe larger Patterns particles offrom the 2.5 Particle to >10.0 Concentration µm gradually and declined Meteorological during the Data working hours before peaking at midnight and then tended to slightly increase in the night time. The particle number size distributions in six size ranges (0.3 to >10 µm) were collected during the measurementTable 4. Summary period of as the shown particle innumber Table size4. Thedistribu hourlytions across averaged the measurement values of periods. the particle Period number sizes are1 shown = 07:00–19:00, in Figure Period6 .2 It= 19:00–23:00, was found Period that 3 the= 23:00–07:00. diurnal tendencies of the measured PNC were different depending on the particle size. In general, there are two temporal patterns for the particle Particle Number Size Ranges [µm] sizes. SmallerPeriod particles between0.3–0.5 0.3 and 1.00.5–1.0µm tended1.0–2.5 to decrease2.5–5.0 during 5.0–10.0 the periods >10.0 of 0:00–02:00 and 21:00–23:00P1 and tendedMean to197,966 peak around 24,725 noon (11:00–12:00). 1,642 In 108contrast to 50 the smaller 9 particles, the larger particles from 2.5Min to >10.0175,560µm gradually21,208 declined1,365 during the 86 working 36 hours before 6 peaking at midnight and then tendedMax to slightly216,635 increase27,992 in the night1,934 time. 140 70 15 SD 9427 1574 136 9 7 2 P2 Mean 179,809 23,593 1,339 111 57 11 Min 149,664 20,829 1,157 93 44 8 Max 206,362 27,531 1,758 152 84 16 SD 16,328 1761 145 14 9 2 P3 Mean 174,314 22,045 1,651 137 71 13 Min 147,226 17,939 1,198 101 52 9 Max 206,081 26,070 2,073 235 132 27 SD 17,885 2511 186 22 15 3 Total Mean 187,056 23,643 1,594 118 58 11 Min 147,226 17,939 1,157 86 36 6 Sustainability 2018, 10, 4599 9 of 19

Table 4. Summary of the particle number size distributions across the measurement periods. Period 1 = 07:00–19:00, Period 2 = 19:00–23:00, Period 3 = 23:00–07:00.

Particle Number Size Ranges [µm] Period 0.3–0.5 0.5–1.0 1.0–2.5 2.5–5.0 5.0–10.0 >10.0 P1 Mean 197,966 24,725 1,642 108 50 9 Min 175,560 21,208 1,365 86 36 6 Max 216,635 27,992 1,934 140 70 15 SD 9427 1574 136 9 7 2 P2 Mean 179,809 23,593 1,339 111 57 11 Sustainability 2018,Min 10, x FOR PEER 149,664 REVIEW 20,829 1,157 93 44 8 9 of 18 Max 206,362 27,531 1,758 152 84 16 SDMax 16,328216,635 176127,992 2,073 145 235 14 132 927 2 SD 17,794 2296 193 20 14 3 P3 Mean 174,314 22,045 1,651 137 71 13 Table 5 presents the measured meteorological indicators across three measurement periods. Min 147,226 17,939 1,198 101 52 9 During the sampling period, the ambient temperature was almost constant in the range from 5.0 to Max 206,081 26,070 2,073 235 132 27 6.1 °C (mean = SD5.2 °C, SD 17,885= 0.3 °C) as shown 2511 in Figure 1867a. The wind speed 22 showed 15 small variations 3 ranging from 0.0–0.5 m/s, as plotted in Figure 7b. Additionally, there was no wind during the Total Mean 187,056 23,643 1,594 118 58 11 measurement period of 12:00–22:00. According to the Beaufort wind-force scale [47], the wind speed Min 147,226 17,939 1,157 86 36 6 (mean = 0.2 m/s, SD = 0.2 m/s) across the measurement period can be described as calm. RH showed Max 216,635 27,992 2,073 235 132 27 large variation SDduring the 17,794 measurement 2296 period as shown 193 in Figure 207c. In Period 14 1, RH decreased 3 from 54.4% to 39.6%. During period 1 and 2, RH gradually increased by 58.5%.

FigureFigure 6. Temporal 6. Temporal patterns patterns of of the the particle particle numbernumber concentrations.concentrations. The The error error bars bars indicate indicate the the standardstandard deviations. deviations.

TableTable5 presents 5. Summary the of measured the meteorological meteorological indicators acro indicatorsss the measurement across threeperiods. measurement Period 1 = 07:00– periods. During the19:00, sampling Period 2 period,= 19:00–23:00, the ambientPeriod 3 = 23:00–07:00. temperature was almost constant in the range from 5.0 to 6.1 ◦C (mean = 5.2 ◦C,Period SD = 0.3 ◦C) as shown Wind inSpeed Figure [m/s]7a. The Temp. wind [°C] speed RH showed [%] small variations ranging from 0.0–0.5 m/s,P1 asMean plotted in Figure 0.17 b. Additionally, 5.3 there was 41.1 no wind during the measurement period of 12:00–22:00.Min According 0.0 to the Beaufort wind-force 5.0 scale 30.8 [47], the wind speed (mean = 0.2 m/s, SD = 0.2 m/s)Max across the measurement 0.6 period can 6.6 be described 58.0 as calm. RH showed large variation during the measurementSD period as 0.2 shown in Figure 0.47 c. In Period 6.0 1, RH decreased from P2 Mean 0.1 5.2 42.3 54.4% to 39.6%. During period 1 and 2, RH gradually increased by 58.5%. Min 0.0 4.9 38.5 Max 1.1 5.6 46.0 SD 0.2 0.2 2.2 P3 Mean 0.4 5.1 52.8 Min 0.0 4.9 45.1 Max 0.6 5.1 61.0 SD 0.2 0.1 4.3 Total Mean 0.2 5.2 45.2 Min 0.0 4.9 30.8 Max 1.1 6.6 61.0 SD 0.3 0.3 7.4 Sustainability 2018, 10, 4599 10 of 19

Table 5. Summary of the meteorological indicators across the measurement periods. Period 1 = 07:00–19:00, Period 2 = 19:00–23:00, Period 3 = 23:00–07:00.

Period Wind Speed [m/s] Temp. [◦C] RH [%] P1 Mean 0.1 5.3 41.1 Min 0.0 5.0 30.8 Max 0.6 6.6 58.0 SD 0.2 0.4 6.0 P2 Mean 0.1 5.2 42.3 Min 0.0 4.9 38.5 Max 1.1 5.6 46.0 SD 0.2 0.2 2.2 P3 Mean 0.4 5.1 52.8 Min 0.0 4.9 45.1 Max 0.6 5.1 61.0 SD 0.2 0.1 4.3 Total Mean 0.2 5.2 45.2 Min 0.0 4.9 30.8 Max 1.1 6.6 61.0 SD 0.3 0.3 7.4 Sustainability 2018, 10, x FOR PEER REVIEW 10 of 18

Figure 7.FigureTemporal 7. Temporal patterns patterns of the of meteorologicalthe meteorological conditions: conditions: ( aa)) wind wind speed, speed, (b) ( btemperature,) temperature, and and (c) relative( humidity.c) relative humidity.

3.4. Relationships between Noise Levels and Traffic Data Correlation analyses between the noise parameters and traffic data were conducted using the measured data. The correlation coefficients between the noise indicators and traffic volume for each road are presented in Table 6 according to the vehicle types. In addition, the correlation between the noise indicators and traffic speed are listed in Table 7. In general, there was a reverse relationship between the traffic volume and traffic speed. This indicates that the traffic speed tended to decrease as the traffic volume increased on a road due to traffic congestion. Overall, Leq is highly correlated with the traffic volume and traffic speed on T1 and T2, which are close to the measurement point, whereas Leq showed a relatively lower correlation with traffic on T3, which is more than 300 m from the measurement unit. Similarly, more significant correlations between the percentile levels and traffic parameters were found on T1 and T2 compared to T3. Among the percentile noise levels, L90, closely related to the level, showed the highest correlation with the traffic parameters across three traffic roads. The traffic volume of the subway exhibited similar correlation patterns with the noise indicators compared to road traffic, showing positive correlations with Leq and LOLF, but negative correlation with LHF-LF. Regarding the vehicle types, the correlations for light vehicle volumes were generally greater than those for heavy vehicle volumes. This may be because the proportions of light vehicles were Sustainability 2018, 10, 4599 11 of 19

3.4. Relationships between Noise Levels and Traffic Data Correlation analyses between the noise parameters and traffic data were conducted using the measured data. The correlation coefficients between the noise indicators and traffic volume for each road are presented in Table6 according to the vehicle types. In addition, the correlation between the noise indicators and traffic speed are listed in Table7. In general, there was a reverse relationship between the traffic volume and traffic speed. This indicates that the traffic speed tended to decrease as the traffic volume increased on a road due to traffic congestion.

Table 6. Correlation coefficients between the noise levels and traffic volume.

Road Vehicle Type Leq L90 L50 L10 LOLF LHLF LHF-LF Light 0.72 ** 0.82 ** 0.74 ** 0.72 ** 0.79 ** −0.51 * −0.79 ** T1 Heavy 0.71 ** 0.77 ** 0.70 ** 0.70 ** 0.70 ** −0.49 * −0.71 ** Total 0.73 ** 0.83 ** 0.75 ** 0.73 ** 0.79 ** −0.51 * −0.79 ** Light 0.72 ** 0.83 ** 0.75 ** 0.72 ** 0.75 ** −0.39 −0.73 ** T2 Heavy 0.48 * 0.66 ** 0.53 ** 0.48 * 0.54 ** −0.24 −0.51 ** Total 0.69 ** 0.82 ** 0.73 ** 0.70 ** 0.73 ** −0.38 −0.71 ** Light 0.49 * 0.62 ** 0.52 ** 0.50 * 0.76 ** −0.22 −0.70 ** T3 Heavy 0.10 0.22 0.13 0.09 0.04 0.05 −0.02 Total 0.49 * 0.63 ** 0.53 ** 0.50 * 0.74 ** −0.21 −0.67 ** Subway Train 0.62 ** 0.77 ** 0.67 ** 0.63 ** 0.75 ** −0.36 −0.72 ** * p < 0.05, ** p < 0.01.

Table 7. Correlation coefficients between the noise levels and traffic speed.

Road Leq L90 L50 L10 LOLF LHLF LHF-LF T1 −0.80 ** −0.83 ** −0.80 ** −0.81 ** −0.80 ** 0.60 ** 0.81 ** T2 −0.50 ** −0.64 ** −0.55 ** −0.51 ** −0.68 ** 0.24 * 0.63 ** T3 −0.59 ** −0.60 ** −0.59 ** −0.60 ** −0.72 ** 0.52 ** 0.73 ** * p < 0.05, ** p < 0.01.

Overall, Leq is highly correlated with the traffic volume and traffic speed on T1 and T2, which are close to the measurement point, whereas Leq showed a relatively lower correlation with traffic on T3, which is more than 300 m from the measurement unit. Similarly, more significant correlations between the percentile levels and traffic parameters were found on T1 and T2 compared to T3. Among the percentile noise levels, L90, closely related to the background noise level, showed the highest correlation with the traffic parameters across three traffic roads. The traffic volume of the subway exhibited similar correlation patterns with the noise indicators compared to road traffic, showing positive correlations with Leq and LOLF, but negative correlation with LHF-LF. Regarding the vehicle types, the correlations for light vehicle volumes were generally greater than those for heavy vehicle volumes. This may be because the proportions of light vehicles were significantly larger than those of heavy vehicles across the three road sections, meaning the contributions of light vehicles to the variations in noise indicators may be more significant than those of heavy vehicles in the measurement locations for our study. The spectral characteristics of noise were also associated with the traffic parameters. The LOLF values representing low frequency levels generated from vehicle are positively correlated with traffic volumes, while a negative relationship was obtained for the traffic speed (p < 0.01). Conversely, the LHLF values related to high frequencies from rolling noise showed statistically negative and positive correlations with the traffic volume and traffic speed, respectively, for all of the traffic roads. This can be explained because noise levels at low frequencies tend to increase with increasing traffic volume, which causes low vehicle speeds. On the contrary, increasing traffic speed may cause increased rolling noise, which is closely related to the SPLs in the range of 1–2 kHz. Sustainability 2018, 10, 4599 12 of 19

In particular, traffic data, such as volume and speed on T1, showed slightly stronger correlations with LOLF compared to those on T2. This may be because lower traffic speeds on T1 (mean traffic: 25.3 km/h) lead to lower-frequency contributions compared to T2 (mean traffic: 37.4 km/h) because the noise of the /pavement interface typically dominates at 40 km/h or greater [48]. The correlations between LOLF and the traffic parameters were relatively stronger than those of LHLF. This may be because road traffic noise mainly consists of low frequency contents. The LHF-LF value, which represents the relative contribution of high frequency energy to low frequencies, was highly correlated with the traffic parameters. Although the mean traffic speed on T3 was high at approximately 80 km/h, which may contribute to noise above 1 kHz being generated by the tire/pavement interface, the correlations between the traffic speed on T1 and high-frequency noise indicators (LHLF and LHF-LF) were relatively stronger than those on T3. This can be explained by the fact that the contributions of T3 to LHLF and LHF-LF may have been shielded by the nearby road T1, which dominated the noise indicators, because T3 was much farther away from the measurement location than the other road sections.

3.5. Relationships between the PNC, Traffic Data, and Meteorological Data The correlation coefficients between the PNCs and traffic parameters (traffic volume and speed) are listed in Tables8 and9, respectively. Two major relationships were found in terms of particle size. Smaller particle sizes ranging from 0.3–1.0 µm showed a strong positive correlation with the traffic volume on T1 and T2 for both light and heavy vehicles, whereas the correlation coefficients between submicron particles (0.3–1.0 µm) and the traffic volumes on T3 and the subway lane were not significant. Statistically significant correlations were only found between the traffic volumes of heavy vehicles and particle sizes of 0.3–0.5 µm (r = 0.47, p < 0.05) and 1.0–2.5 µm (r = 0.50, p < 0.05). Overall, statistically significant correlations were not observed between traffic speed and the concentration of smaller particles on the three road sections, except for particle sizes of 0.3–0.5 µm on T3 (r = −0.41, p < 0.05). These findings indicate that the concentrations of submicron particles were significantly influenced by traffic volume on roads near the measurement unit. Statistically significant correlations were not found between particles with sizes of 1.0–2.5 µm and traffic parameters, except for the relationship with the traffic speed on T3 (r = 0.66, p < 0.01).

Table 8. Correlation coefficients between the PNC and traffic volume.

Particle Size Range [µm] Road Vehicle Type 0.3–0.5 0.5–1.0 1.0–2.5 2.5–5.0 5.0–10.0 >10.0 Light 0.60 ** 0.52 ** −0.05 −0.74 ** −0.74 ** −0.70 ** T1 Heavy 0.65 ** 0.56 ** 0.08 −0.69 ** −0.72 ** −0.69 ** Total 0.62 ** 0.54 ** −0.03 −0.74 ** −0.75 ** −0.71 ** Light 0.53 ** 0.49 * −0.06 −0.68 ** −0.67 ** −0.63 ** T2 Heavy 0.56 ** 0.42 * 0.16 −0.59 ** −0.64 ** −0.66 ** Total 0.55 ** 0.49 * −0.02 −0.68 ** −0.68 ** −0.65 ** Light 0.20 0.33 −0.29 −0.64 ** −0.59 ** −0.51 * T3 Heavy 0.47 * 0.38 0.50 * −0.15 −0.30 −0.40 Total 0.25 0.36 −0.22 −0.63 ** −0.60 ** −0.54 ** Subway Train 0.38 0.36 −0.33 −0.64 ** −0.60 ** −0.56 ** * p < 0.05, ** p < 0.01. Sustainability 2018, 10, 4599 13 of 19

Table 9. Correlation coefficients between the PNC and traffic speed.

Particle Size Range [µm] Road 0.3–0.5 0.5–1.0 1.0–2.5 2.5–5.0 5.0–10.0 >10.0 T1 −0.41 * −0.34 0.30 0.52 ** 0.45 * 0.35 * T2 −0.12 −0.11 0.34 0.56 ** 0.48 * 0.39 * T3 −0.13 −0.24 0.66 ** 0.45 * 0.33 0.22 * p < 0.05, ** p < 0.01.

The PNC for particles larger than 2.5 µm was more significantly correlated with traffic data including traffic volume and speed than smaller particle sizes of 0.3–1.0 µm. In contrast to submicron particle sizes, larger particle sizes (2.5–10 µm) had negative correlations with traffic volumes for all three road sections and the subway lane. It was also found that the correlation of traffic volume increased as the distance from the measurement position decreased. The correlation strengths between particles larger than 2.5 µm and traffic volume on T1 and T2 were relatively stronger than that on T3. This implies that the distance from the traffic road may be one of the factors that affects the PNC. In terms of vehicle types, the correlation coefficients for the light and heavy vehicle types on T1 and T2 were similar. Unlike T1 and T2, the traffic volume of light vehicles on T3 was significantly correlated to the PNCs (2.5–10 µm), whereas that of heavy vehicles on T3 did not show any significant relationship with larger particle sizes (2.5–10 µm). In addition, positive relationships were also found between the number of larger particles (>2.5 µm) and the traffic speed on T1 and T2, whereas the particles between 2.5 and 5.0 µm only showed a statistically significant correlation with the traffic speed on T3. In particular, the correlation between the PNC and traffic speed decreased as the particle size increased. Among the larger particles, the particles with sizes of 2.5–5.0 µm were the most significantly correlated with traffic speed for all of the roads. Table 10 presents the correlation coefficients between the PNC and meteorological conditions. Overall, the correlation strengths of meteorological parameters were weaker than those of the noise parameters. Wind speed and RH showed negative correlations with the PNC at <1.0 µm, with a positive correlation with larger particle sizes (>2.5 µm). In terms of temperature, negative relationships with the particle size (1.0–10.0 µm) were found and the correlations with the PNC were weaker compared to those of the RH and wind speed.

Table 10. Correlation coefficients between the PNC and meteorological data.

Particle Size Range [µm] Factor 0.3–0.5 0.5–1.0 1.0–2.5 2.5–5.0 5.0–10.0 >10.0 Wind speed −0.33 ** −0.36 ** 0.26 ** 0.34 ** 0.28 ** 0.19 ** Temperature 0.34 ** 0.09 −0.27 ** −0.19 ** −0.11 * −0.04 RH −0.40 ** −0.31 ** 0.32 ** 0.47 ** 0.40 ** 0.29 ** * p < 0.05, ** p < 0.01.

3.6. Relationships between Noise Indicators and Particle Number Concentration Correlation analyses between the noise parameters and PNCs was carried out and the results are listed in Table 11. It was found that the correlation tendencies between the noise parameters and PNC differed according to the particle size implying that appropriate noise parameters to represent the PNC may differ depending on the particle size. Sustainability 2018, 10, 4599 14 of 19

Table 11. Correlation coefficients between the noise levels and particle number concentration.

Particle Size Range Leq L90 L50 L10 LOLF LHLF LHF-LF 0.3–0.5 µm 0.61 ** 0.57 ** 0.58 ** 0.61 ** 0.36 ** −0.62 ** −0.47 ** 0.5–1.0 µm 0.56 ** 0.50 ** 0.52 ** 0.57 ** 0.43 ** −0.59 ** −0.51 ** 1.0–2.5 µm −0.07 −0.10 −0.10 −0.08 −0.30 ** 0.04 0.27 ** 2.5–5.0 µm −0.53 ** −0.55 ** −0.53 ** −0.52 ** −0.62 ** 0.35 ** 0.63 ** 5.0–10.0 µm −0.54 ** −0.56 ** −0.53 ** −0.53 ** −0.60 ** 0.36 ** 0.61 ** >10.0 µm −0.49 ** −0.51 ** −0.48 ** −0.48 ** −0.51 ** 0.33 ** 0.52 ** ** p < 0.01.

The PNCs for particle sizes of 0.3–1.0 µm showed statistically positive relationships with Leq and the percentile noise levels, whereas negative correlations were observed for particles larger than 2.5 µm. Significant correlations were not observed between Leq and particle sizes of 1.0–2.5 µm. Similarly, LOLF had positive and negative correlations with particle sizes in the range of 0.3–2.5 µm and larger than 2.5 µm, respectively. These results can be explained by the correlations between traffic parameters, noise indicators, and particle sizes of the PNCs in this study, as illustrated in Figure8. The PNCs of larger particle sizes (>2.5 µm) showed positive correlations with traffic speed, as shown in Table5. The noise indicators Leq and LOLF had strong negative correlations with traffic speed and larger particles (>2.5 µm), as shown in Table3. Based on these relationships, one can see that the Leq and LOLF could beSustainability utilized as2018 noise, 10, x indicatorsFOR PEER REVIEW to predict the PNCs of larger particles (>2.5 µm). 14 of 18

FigureFigure 8.8.Summary Summary ofof relationshipsrelationships betweenbetween traffictraffic parameters,parameters, noisenoise indicators,indicators, andand PNCsPNCs basedbased onon ourour measurements.measurements.

4. DiscussionsIn contrast to LOLF and Leq, the high-frequency noise indicators LHLF and LHF-LF showed negative correlations with submicron particles (0.3–1.0 µm), but positive correlations with particles larger than Based on in-situ measurements carried for 24 h, it was revealed that there are significant 2.5 µm. As illustrated in Figure8, the traffic volume on closer road sections showed positive correlation correlations among the noise levels, PNC, and traffic parameters. Overall, traffic closer to the with the PNCs of submicron particles (0.3–1.0 µm). Additionally, it was found that high-frequency measurement position, as is the case with T1 and T2, had more of an influence on the noise parameters noise indicators were negatively associated with traffic volume. These findings indicate that LHLF and and PNC than the distant expressway, T3. Even though the traffic parameter at T3 is much greater LHF-LF can be utilized to predict the PNCs of submicron particles (0.3–1.0 µm). than the other roads, the traffic on T3 mainly contributes to stationary background noise levels and the PNC for the measurement site. This indicates that local variations of the noise levels and particle distributions may be influenced by not only the traffic volume but also the distance from the roads. It was observed that the temporal patterns of noise, traffic, and PNC varied depending on the time of day or night. This finding was in good agreement with the results of previous studies in which there are significant differences of noise and air pollutants between day and night [40,42]. Interestingly, the relationship between the noise parameters and PNC also differed according to the particle size. To evaluate the extent of the correlations among the noise and PNC according to the day and night time periods, the correlation coefficients were calculated, as presented in Table 12. According to EEA, daytime is defined as the hours from 07:00 until 22:00 and nighttime is the period from 22:00–07:00. The particle numbers were aggregated in terms of particle sizes in the ranges of 0.3–1.0 µm and >2.5 µm. With regards to noise parameters, the overall noise level (Leq) and low frequency noise level (LOLF) showed positive correlations with the PNC at 0.3–1.0 µm during the daytime, while significant correlations were not found between the noise parameters and submicron particles during the nighttime. These findings demonstrate that the submicron particles are strongly related to traffic volumes at daytime. Only the high frequency noise level (LHLF) exhibited strong and negative correlations with the number of submicron particles (r = −0.70, p < 0.01). This may be because of the noise emissions spectra of vehicles with high traffic speeds and less confounding by other ambient noise sources in nighttime periods [42]. The PNC with particles larger than 2.5 µm was strongly correlated with the low and high frequency characteristics of the noises and the correlations during the day and night. The correlation Sustainability 2018, 10, 4599 15 of 19

4. Discussion Based on in-situ measurements carried for 24 h, it was revealed that there are significant correlations among the noise levels, PNC, and traffic parameters. Overall, traffic closer to the measurement position, as is the case with T1 and T2, had more of an influence on the noise parameters and PNC than the distant expressway, T3. Even though the traffic parameter at T3 is much greater than the other roads, the traffic on T3 mainly contributes to stationary background noise levels and the PNC for the measurement site. This indicates that local variations of the noise levels and particle distributions may be influenced by not only the traffic volume but also the distance from the roads. It was observed that the temporal patterns of noise, traffic, and PNC varied depending on the time of day or night. This finding was in good agreement with the results of previous studies in which there are significant differences of noise and air pollutants between day and night [40,42]. Interestingly, the relationship between the noise parameters and PNC also differed according to the particle size. To evaluate the extent of the correlations among the noise and PNC according to the day and night time periods, the correlation coefficients were calculated, as presented in Table 12. According to EEA, daytime is defined as the hours from 07:00 until 22:00 and nighttime is the period from 22:00–07:00. The particle numbers were aggregated in terms of particle sizes in the ranges of 0.3–1.0 µm and >2.5 µm.

Table 12. Correlation coefficients between the noise parameters and PNC for the daytime (07:00–22:00) and nighttime (23:00–06:00).

PNC Period Leq LOLF LHLF LHF-LF Day 0.54 ** 0.16 * −0.43 ** −0.27 ** 0.3–1.0 µm Night −0.02 −0.14 −0.70 ** −0.03 Day −0.19 ** −0.34 ** 0.05 0.30 ** >2.5 µm Night −0.32 ** −0.29 ** 0.20 0.34 ** * p < 0.05, ** p < 0.01.

With regards to noise parameters, the overall noise level (Leq) and low frequency noise level (LOLF) showed positive correlations with the PNC at 0.3–1.0 µm during the daytime, while significant correlations were not found between the noise parameters and submicron particles during the nighttime. These findings demonstrate that the submicron particles are strongly related to traffic volumes at daytime. Only the high frequency noise level (LHLF) exhibited strong and negative correlations with the number of submicron particles (r = −0.70, p < 0.01). This may be because of the noise emissions spectra of vehicles with high traffic speeds and less confounding by other ambient noise sources in nighttime periods [42]. The PNC with particles larger than 2.5 µm was strongly correlated with the low and high frequency characteristics of the noises and the correlations during the day and night. The correlation strengths during the day and night were not significantly different. This implies that the relationship between the PNC at >2.5 µm and noise parameters were consistent over the whole measurement period. Stepwise multiple regression analyses were conducted using a linear combination of noise and meteorological parameters to obtain optimal models to estimate the PNC depending on the particle size. Equations (1) and (2) show the prediction models of PNC for 0.3–1.0 µm and >2.5 µm particles with standardized regression coefficients, respectively. As shown in Equation (1), three variables, LHLF, Leq, and RH, were selected to estimate the PNC for submicron particles. The regression model could explain approximately 54% of the variance in the PNC for particle sizes in the range of 0.3–1.0 µm. The standardized partial regression coefficients for LHLF, Leq, and RH were −0.54, 0.55, and 0.33, respectively. This indicates that the contributions of LHLF and Leq to the PNC (0.3–1.0 µm) are similar, while the influence of the RH is relatively small. As shown in Equation (2), the stepwise regression model for larger particles showed that LOLF and Leq are significant predictors for the PNC of particles 2 >2.5 µm (R = 0.40). Particularly, the contribution of LOLF in the estimation of the PNC (>2.5 µm) is twice as large as that of Leq. These findings indicate that the noise parameters representing the overall Sustainability 2018, 10, 4599 16 of 19 levels and frequency characteristics of noise may be used to explain the relationship between noise and air pollution in urban areas.

2 PNC0.3–1.0 µm ≈ −0.54LHLF + 0.55Leq + 0.33 RH (R = 0.54, p < 0.001) (1)

2 PNC>2.5 µm ≈ −0.46LOLF − 0.23Leq (R = 0.40, p < 0.001) (2)

5. Conclusions Based on field measurements obtained over 24 h in an urban area, strong correlations between noise, traffic, and PNC were revealed. Traffic parameters, including volume and speed, affected both the noise and PNC, confirming that they are common sources of noise and air pollution. In particular, the spectral characteristics of noise were closely associated with traffic volume and speed, which also showed significant correlations with PNC. The relationship between the noise and PNC differed depending on the particle size. Regarding noise indicators, PNC (0.3–1.0 µm) showed stronger correlations with LHLF, whereas LOLF had stronger correlations with larger particles (>2.5 µm). The overall noise level Leq showed significant correlations with both smaller (0.3–1.0 µm) and larger (>2.5 µm) PNCs. PNC (0.3–1.0 µm) showed a stronger correlation with noise during the daytime, but relatively consistent relationships were observed between the PNC (>2.5 µm) and noise parameters for both day and night periods. These results support the idea that frequency-specific noise indicators and traffic data provide useful knowledge regarding the relationships between noise and air pollutants in urban environments. Furthermore, the findings of this study demonstrate the importance of monitoring temporally-resolved and spectral-specific air and noise pollutants to better understand community exposure and the health impacts of air and noise pollution. Despite the significance of our findings, inherent limitations remain in our study. A measurement period of 24 h limits our ability to characterize the relationships between noise, traffic, and air pollution. Therefore, long-term studies across multiple seasons and spaces are required to validate these relationships. Additionally, some factors that might affect noise and air pollution were not considered in this present study. For example, although the distance to road sections could play a key role in noise and air pollution, the effects of the distances of sources were not explored in depth because our measurement location considered three road sections at different distances. Therefore, the relationship between the distance to a road section and PNCs should be investigated in the future. Furthermore, vehicle compositions (e.g., proportions of light and heavy vehicles on road sections) and the fuel types of vehicles (e.g., electric, diesel, or gasoline vehicles) could be critical factors in future studies because the emission rate of both the frequency content of noise and particulate matter varies according to the types of vehicles and fuel types. Finally, it should be noted that some results may be masked by other sources of air-noise pollution near the measurement location, which were not identified in this study.

Author Contributions: Conceptualization, J.Y.J., J.Y.H. and K.H.K.; Data curation, K.H.K.; Formal analysis, J.Y.H and S.M.K.; Methodology, J.Y.H.; Writing—original draft, J.Y.H; Writing—review & editing, J.Y.H., S.M.K., and J.Y.J. Funding: This work was supported by a grant the Global Frontier R&D Program on “Human-centered Interaction for Coexistence,” from the National Research Foundation of Korea which was funded by the Korean government (MSIP) (2013M3A6A3079356). Conflicts of Interest: The authors declare no conflict of interest.

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